Skip to content
DraconiticResearch
Search Sources API
189,105 studies31 sourcesUpdated 12 min ago
PreprintCC BY 4.0arXiv

On one-dimensional pressureless Euler--Poisson systems: existence for non-semiconvex interaction potentials

Abstract

One-dimensional Euler-Poisson-type systems with interaction potentials that are repulsive at short range and attractive at long range are useful simplified models that describe biological aggregation. In the current work we employ new techniques to treat compactly supported solutions in the case where the potential is C1 and satisfies certain coercivity growth conditions although it is not necessarily semiconvex, as required in previous work. Central to this approach are uniform bounds on the positions and velocities of discrete sticky-particle solutions to such a system, which requires the potential be only C0, 1loc. In the semiconvex case, these bounds also yield convergence of time-shifted trajectories to an eternal solution. The tradeoff, just as in the case of repulsive Euler-Poisson, is that we cannot claim that the emerging solutions for non-semiconvex potentials are sticky.

Related

  1. Global existence and time decay for a bipolar Euler-Poisson system with one pressureless and undamped fluid
    Young-Pil Choi, Houzhi Tang, Weiyuan Zou
    arXivPreprintCC BY 4.0Full textAnalysis & PDEsarXiv
  2. Global Dynamic Patterns of Entropy Solutions for One-dimensional Pressureless Euler System
    Gaowei Cao, Kai Hu, Feimin Huang +1
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  3. One-dimensional pressureless flow with a nonlinear velocity law: Bregman variational construction and well-posedness
    Gaowei Cao, Feimin Huang, Guirong Tang
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  4. Sharp existence and non-existence for singular $1$-Laplace equations with Hardy potentials
    Juan Carlos Chata Ortiz, Francesco Petitta
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  5. Existence of ground state solutions to Kirchhoff--Choquard system in ℝ3 with nonconstant potentials
    Hiroshi Matsuzawa
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
BibTeX
@misc{xie2026onedimensional,
  title = {{On one-dimensional pressureless Euler--Poisson systems: existence for non-semiconvex interaction potentials}},
  author = {Andrew Xie and Emmanuel Alayande and Christopher Chun and Yusen Li and Rohan Mawalkar and Adrian Tudorascu and Adam Van},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.25754},
  eprint = {2610.25754},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.25754},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - On one-dimensional pressureless Euler--Poisson systems: existence for non-semiconvex interaction potentials
AU  - Andrew Xie
AU  - Emmanuel Alayande
AU  - Christopher Chun
AU  - Yusen Li
AU  - Rohan Mawalkar
AU  - Adrian Tudorascu
AU  - Adam Van
PY  - 2026
DA  - 2026/10/21
PB  - arXiv
DO  - 10.48550/arxiv.2610.25754
UR  - https://arxiv.org/abs/2610.25754
AB  - One-dimensional Euler-Poisson-type systems with interaction potentials that are repulsive at short range and attractive at long range are useful simplified models that describe biological aggregation. In the current work we employ new techniques to treat compactly supported solutions in the case where the potential is C^1 and satisfies certain coercivity growth conditions although it is not necessarily semiconvex, as required in previous work. Central to this approach are uniform bounds on the positions and velocities of discrete sticky-particle solutions to such a system, which requires the potential be only C^0, 1_loc. In the semiconvex case, these bounds also yield convergence of time-shifted trajectories to an eternal solution. The tradeoff, just as in the case of repulsive Euler-Poisson, is that we cannot claim that the emerging solutions for non-semiconvex potentials are sticky.
ER  -